Transcript Slide 1
NGC 2110 Spectroscopy Dan Evans (Harvard), Julia Lee (Harvard), Jane Turner (UMBC/GSFC), Kim Weaver (GSFC), Herman Marshall (MIT) NGC 2110 Spectroscopy Fe Kα Lines and Reflection: AGN Geometry • The Fe Kα line complex in general consists of a narrow line core, possibly accompanied by broadened emission • What is the origin of the broad emission? • • • • • • Relativistically blurred diskline? Compton shoulder? Broad line region? Unmodeled absorption? If we can deconvolve the contributions from the two, we can probe AGN geometry Vital to treat direct+reflected continuum and absorption effects self-consistently Diskline? Compton shoulder? Complex absorption? NGC 3783 (Yaqoob et al. 2005) Nearby (z=0.0076, DL=33 Mpc) NELG • Historical subclass of Seyferts with narrow (<600 km/s) optical lines (Sy 2-like) but much stronger hard X-ray emission (Sy 1-like) • Flat X-ray spectra may imply they dominate XRB at low energies (e.g. Iwasawa et al. 1997) • Transitional between Sy 1 and Sy 2? (Lawrence & Elvis 1982) ASCA, BeppoSAX, etc. 2-10 keV X-ray spectrum is very flat (Г=1.4) • Accompanied by moderate absorption (NH=3x1022 cm-2) ASCA Fe K complex hard to interpret • Diskline, either oriented at intermediate angles to l.o.s. (Weaver & Reynolds 1998) or nearly face-on (Turner et al. 1998) NGC 2110 Spectroscopy NGC 2110 NGC 2110 Spectroscopy NGC 2110 was observed with Chandra for a total of 250 ks and XMM-Newton for 60 ks. An initial analysis showed variability in flux only, and so the continuum spectra were analyzed jointly. Instrument Date Exposure (ks) HETGS 2001 Dec 19 35 HETGS 2001 Dec 20 80 HETGS 2001 Dec 22 35 HETGS 2003 Mar 05 100 EPIC/RGS 2003 Mar 05 60 2003 Mar HETGS light curve 2001 Dec NGC 2110 Spectroscopy Chandra and XMM-Newton • • Initial fit with single, moderately absorbed power law (NH=3x1022 cm2, Г=1.4) Soft excess seen below 2 keV • Significant improvement in fit with the addition of a lightly absorbed (NH=7x1020 cm-2) power law (Гsoft=Гhard) • Still very flat photon index (Г=1.4), but… XMM pn MEG XMM pn MEG NGC 2110 Spectroscopy Continuum Fitting • Insufficient opacity at Si K and Fe K edges • Improvement in the fit with the additional edges • Does this imply an extra absorber? • Significant improvement with a 3x partially covered power law • • HEG XMM pn Photon index rises to Г=1.74±0.05 consistent with canonical values in Seyferts MEG HEG No evidence for ionized absorption in HETGS data Component Column density (cm-2) Covering fraction NH,1 1.6x1023 32% NH,2 2.8x1022 65% NH,3 7.7x1020 3% NGC 2110 Spectroscopy Continuum Fitting • Chandra HETGS best suited to probe narrow lines • Neutral fluorescent Kα lines detected from Si, S, Ar, Ca, Fe • Narrow Fe Kα and Si Kα line cores just resolved with HETGS Line Energy (keV) Width (km s-1) Equivalent width (eV) Fe Kα 6.397±0.007 900±500 80±30 Si Kα 1.740±0.002 600±400 6±2 • Distant, neutral fluorescing region • No evidence for diskline • Marginal (2.5σ) evidence for v. slight broadened base of Fe Kα HEG HEG NGC 2110 Spectroscopy Fluorescent Line Diagnostics NGC 2110 Spectroscopy Reflection • Self-consistent treatment of reflection (i.e., lines+pexrav continuum) • No change in fit parameters • Suzaku provides vital constraints on strength of reflection • Stringent limit of R<0.1 (Reeves et al. 2006; Okajima et al. 2007) • NGC 2110 is one of the few Seyferts with no evidence for disk reflection, nor complex absorption Suzaku – NGC 2110 (Reeves et al. 2006) NGC 2110 Spectroscopy • Excellent spatial agreement between X-ray and [OIII] (Evans et al. 2006) • Both clearly offset from radio, but extend along similar p.a. • X-ray & [OIII] emission influenced by, but not directly associated with, radio jet? • ACIS X-ray spectrum modeled by, e.g., two thermal plasma models (kT1=0.3 keV; kT2=5 keV) 2’’=320 pc Chandra (0.5-1.5 keV) / VLA / HST [OIII] NGC 2110 Spectroscopy Multiwavelength Imaging • Evans et al. (2006) considered 3 mechanisms for producing the environment: • • • Shock-heating by the radio jet Electron-scattered nuclear radiation Photoionization by the AGN • High-resolution grating spectroscopy can in principle distinguish between these models • Tentative evidence for O VIII Ly α, as well as the O VIII RRC feature first reported by Guainazzi & Bianchi (2006) • Photoionization and collisional ionization processes both important? NGC 2110 Spectroscopy Gratings Spectrum NGC 2110 Spectroscopy ASCA, BeppoSAX, etc. found • • • Flat (Г=1.4) 2-10 keV spectrum Moderate absorption (NH=3x1022 cm-2) Diskline emission, either face-on or at intermediate angles Component Column density (cm-2) Covering fraction NH,1 1.6x1023 32% NH,2 2.8x1022 65% NH,3 7.7x1020 3% Chandra, XMM-Newton (and Suzaku – Okajima et al. 2007) • • • • • • Compton-thin partial-coverer model Photon index 1.7-1.8 No evidence for ionized absorption Marginally resolved (900±500 km s-1) Fe Kα line core No evidence for disk reflection Multiwavelength imaging + HETGS evidence for (weak) ionized emission extended circumnuclear environment is photoionized or collisionally ionized? 2’’=320 pc NGC 2110 Spectroscopy Recap Consistent with an origin in a Compton-thin, distant (> 1pc) neutral absorber • Orientation consistent with edge-on view • Steepening of photon index using multiple partial-coverer model NELGs do not have significantly flatter spectra w.r.t. Seyfert 1, 2? • No disk reflection, unlike other Compton-thin Seyferts observed with Suzaku (Reeves et al. 2006) • Vital to treat absorption and reflection effects in a self-consistent manner in order to evaluate AGN geometry • High spatial and spectral resolution, together with high effective area, are key to determining the spatial distribution and energetics (collisional vs. photoionization) of circumnuclear environments in AGN NGC 2110 Spectroscopy •